Ultimately, as a byproduct of considering all these definitions, Hayward's
quasilocal action [1]}
\(S_{G}[g]=\frac{1}{16\pi }(\underset{M}{\int }R\omega _{g}+\underset{\Sigma _{1}}{2\overset{\Sigma _{2}}{\int }}K\omega _{h}+2\underset{\mathcal {B}}{\int }\Theta \omega _{\gamma }+\underset{\Omega _{1}}{2\overset{\Omega _{2}}{\int }}\sinh ^{-1}\eta \omega _{q})\) 
